677 research outputs found
Multi-D magnetohydrodynamic modelling of pulsar wind nebulae: recent progress and open questions
In the last decade, the relativistic magnetohydrodynamic (MHD) modelling of
pulsar wind nebulae, and of the Crab nebula in particular, has been highly
successful, with many of the observed dynamical and emission properties
reproduced down to the finest detail. Here, we critically discuss the results
of some of the most recent studies: namely the investigation of the origin of
the radio emitting particles and the quest for the acceleration sites of
particles of different energies along the termination shock, by using wisps
motion as a diagnostic tool; the study of the magnetic dissipation process in
high magnetization nebulae by means of new long-term three-dimensional
simulations of the pulsar wind nebula evolution; the investigation of the
relativistic tearing instability in thinning current sheets, leading to fast
reconnection events that might be at the origin of the Crab nebula gamma-ray
flares.Comment: 30 pages, 12 figure
Fast reconnection in relativistic plasmas: the magnetohydrodynamics tearing instability revisited
Fast reconnection operating in magnetically dominated plasmas is often
invoked in models for magnetar giant flares, for magnetic dissipation in pulsar
winds, or to explain the gamma-ray flares observed in the Crab nebula, hence
its investigation is of paramount importance in high-energy astrophysics. Here
we study, by means of two dimensional numerical simulations, the linear phase
and the subsequent nonlinear evolution of the tearing instability within the
framework of relativistic resistive magnetohydrodynamics, as appropriate in
situations where the Alfven velocity approaches the speed of light. It is found
that the linear phase of the instability closely matches the analysis in
classical MHD, where the growth rate scales with the Lundquist number S as
S^-1/2, with the only exception of an enhanced inertial term due to the thermal
and magnetic energy contributions. In addition, when thin current sheets of
inverse aspect ratio scaling as S^-1/3 are considered, the so-called "ideal"
tearing regime is retrieved, with modes growing independently on S and
extremely fast, on only a few light crossing times of the sheet length. The
overall growth of fluctuations is seen to solely depend on the value of the
background Alfven velocity. In the fully nonlinear stage we observe an inverse
cascade towards the fundamental mode, with Petschek-type supersonic jets
propagating at the external Alfven speed from the X-point, and a fast
reconnection rate at the predicted value R~(ln S)^-1.Comment: 14 pages, 9 figures, accepted for publication (MNRAS
Relativistic Jets and Long-Duration Gamma-ray Bursts from the Birth of Magnetars
We present time-dependent axisymmetric magnetohydrodynamic simulations of the
interaction of a relativistic magnetized wind produced by a proto-magnetar with
a surrounding stellar envelope, in the first seconds after core
collapse. We inject a super-magnetosonic wind with ergs
s into a cavity created by an outgoing supernova shock. A strong
toroidal magnetic field builds up in the bubble of plasma and magnetic field
that is at first inertially confined by the progenitor star. This drives a jet
out along the polar axis of the star, even though the star and the magnetar
wind are each spherically symmetric. The jet has the properties needed to
produce a long-duration gamma-ray burst (GRB). At s after core bounce,
the jet has escaped the host star and the Lorentz factor of the material in the
jet at large radii cm is similar to that in the magnetar wind
near the source. Most of the spindown power of the central magnetar escapes via
the relativistic jet. There are fluctuations in the Lorentz factor and energy
flux in the jet on second timescale. These may contribute to
variability in GRB emission (e.g., via internal shocks).Comment: 5 pages, 3 figures, accepted in MNRAS letter, presented at the
conference "Astrophysics of Compact Objects", 1-7 July, Huangshan, Chin
Relativistic MHD modeling of magnetized neutron stars, pulsar winds, and their nebulae
Neutron stars are among the most fascinating astrophysical sources, being
characterized by strong gravity, densities about the nuclear one or even above,
and huge magnetic fields. Their observational signatures can be extremely
diverse across the electromagnetic spectrum, ranging from the periodic and
low-frequency signals of radio pulsars, up to the abrupt high-energy gamma-ray
flares of magnetars, where energies of ~10^46 erg are released in a few
seconds. Fast-rotating and highly magnetized neutron stars are expected to
launch powerful relativistic winds, whose interaction with the supernova
remnants gives rise to the non-thermal emission of pulsar wind nebulae, which
are known cosmic accelerators of electrons and positrons up to PeV energies. In
the extreme cases of proto-magnetars (magnetic fields of ~10^15 G and
millisecond periods), a similar mechanism is likely to provide a viable engine
for the still mysterious gamma-ray bursts. The key ingredient in all these
spectacular manifestations of neutron stars is the presence of strong magnetic
fields in their constituent plasma. Here we will present recent updates of a
couple of state-of-the-art numerical investigations by the high-energy
astrophysics group in Arcetri: a comprehensive modeling of the steady-state
axisymmetric structure of rotating magnetized neutron stars in general
relativity, and dynamical 3-D MHD simulations of relativistic pulsar winds and
their associated nebulae.Comment: EPS 44th Conference on Plasma Physics (June 2017, Belfast), paper
accepted for publication on Plasma Physics and Controlled Fusio
MHD Interaction of Pulsar Wind Nebulae with SNRs and the ISM
In the late 1960s the discovery of the Crab pulsar in its associated
supernova remnant, launched a new field in supernova remnant research: the
study of pulsar-driven or plerionic supernova remnants. In these type of
remnants, the relativistic wind emitted by the pulsar, blows a pulsar wind
nebula into the interior of its supernova remnant. Now, more then forty years
after the discovery of the Crab pulsar, there are more then fifty plerionic
supernova remnants known, due to the ever-increasing capacity of observational
facilities. I will review our current understanding of the different
evolutionary stages of a pulsar wind nebula as it is interacting with its
associated supernova remnant.Therefore I will discuss both analytical and more
recent numerical (M)HD models.The four main stages of a pulsar wind nebula are:
the supersonic expansion stage, the reverse shock interaction stage, the
subsonic expansion stage and ultimatelythe stage when the head of the bubble is
bounded by a bow shock, due to the supersonic motion of the pulsar. Ultimately
this pulsar wind nebula bow shock will break through its associated remnant,
after which the pulsar-powered bow shock will interact directly with the
interstellar medium. I will discuss recent numerical models from these type of
pulsar wind nebulae and their morphology.Comment: 11 pages, 3 figures, Advances in Space Research, in pres
Polarization in the inner region of Pulsar Wind Nebulae
We present here the first effort to compute synthetic synchrotron
polarization maps of Pulsar Wind Nebulae (PWNe). Our goal is to highlight how
polarization can be used as an additional diagnostic tool for the flow
structure in the inner regions of these nebulae. Recent numerical simulations
suggest the presence of flow velocities ~0.5 c in the surroundings of the
termination shock, where most of the high energy emission comes from. We
construct polarization maps taking into account relativistic effects like
Doppler boosting and position angle swing. The effect of different bulk
velocities is clarified with the help of a toy-model consisting of a uniformly
emitting torus. We also present a map based on recent numerical simulations of
the entire nebula and compare it with presently available data. The comparison
with upcoming high resolution observations could provide new insight into the
inner structure of the nebula and put constraints on the geometrical properties
of the magnetic field.Comment: Accepted for publication on A&A, 6 pages, 2 figure
Local thermodynamical equilibrium and the beta frame for a quantum relativistic fluid
We discuss the concept of local thermodynamical equilibrium in relativistic
hydrodynamics in flat spacetime in a quantum statistical framework without an
underlying kinetic description, suitable for strongly interacting fluids. We
show that the appropriate definition of local equilibrium naturally leads to
the introduction of a relativistic hydrodynamical frame in which the
four-velocity vector is the one of a relativistic thermometer at equilibrium
with the fluid, parallel to the inverse temperature four-vector \beta, which
then becomes a primary quantity. We show that this frame is the most
appropriate for the expansion of stress-energy tensor from local
thermodynamical equilibrium and that therein the local laws of thermodynamics
take on their simplest form. We discuss the difference between the \beta frame
and Landau frame and present an instance where they differ.Comment: 22 pages, 3 figures. To appear in Eur. Phys. J.
Simulated synchrotron emission from Pulsar Wind Nebulae
A complete set of diagnostic tools aimed at producing synthetic synchrotron
emissivity, polarization, and spectral index maps from relativistic MHD
simulations is presented. As a first application we consider here the case of
the emission from Pulsar Wind Nebulae (PWNe). The proposed method is based on
the addition, on top of the basic set of MHD equations, of an extra equation
describing the evolution of the maximum energy of the emitting particles. This
equation takes into account adiabatic and synchrotron losses along streamlines
for the distribution of emitting particles and its formulation is such that it
is easily implemented in any numerical scheme for relativistic MHD. Application
to the axisymmetric simulations of PWNe, analogous to those described by Del
Zanna et al. (2004, A&A, 421, 1063), allows direct comparison between the
numerical results and observations of the inner structure of the Crab Nebula,
and similar objects, in the optical and X-ray bands. We are able to match most
of the observed features typical of PWNe, like the equatorial torus and the
polar jets, with velocities in the correct range, as well as finer emission
details, like arcs, rings and the bright knot, that turn out to arise mainly
from Doppler boosting effects. Spectral properties appear to be well reproduced
too: detailed spectral index maps are produced for the first time and show
softening towards the PWN outer borders, whereas spectral breaks appear in
integrated spectra. The emission details are found to strongly depend on both
the average wind magnetization (here approximately 2%), and on the magnetic
field shape.Comment: 14 pages, submitted to A&
Contribution to Galactic cosmic rays from young stellar clusters
The origin of Galactic cosmic rays (CR) is still a matter of debate.
Diffusive shock acceleration (DSA) applied to supernova remnant (SNR) shocks
provides the most reliable explanation. However, within the current
understanding of DSA several issues remain unsolved, like the CR maximum
energy, the chemical composition and the transition region between Galactic and
extra-Galactic CRs. These issues motivate the search for other possible
Galactic sources. Recently, several young stellar clusters (YSC) have been
detected in gamma rays, suggesting that such objects could be powerful sources
of Galactic CRs. The energy input could come from winds of massive stars hosted
in the clusters which is a function of the cluster total mass and initial mass
function of stars. In this work we evaluate the total CR flux produced by a
synthetic population of YSCs assuming that the CR acceleration occurs at the
termination shock of the collective wind resulting from the sum of cluster's
stellar winds. We show that the spectrum produced by YSC can significantly
contribute to energies TeV if the diffusion inside the wind-blown
bubble is Bohm-like and the spectral slope is harder than the one produced by
SNRs.Comment: Proceeding to the International Cosmic Ray Conference, ICRC 2023,
Nagoya, Japa
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